magnetismo no sistema categorial Graceli

quinta-feira, 1 de novembro de 2018

magnetismo no sistema categorial Graceli.

Matriz categorial de Graceli.

T l T l E l Fl dfG l

N l El tf l

P l Ml tfefel

Ta l Rl

Ll

Dl

Tipos, níveis, potenciais, tempo de ação [categorias de Graceli], temperatura, eletricidade, magnetismo, radioatividade, luminescências, dinâmicas, estruturas, fenômenos, transições de fenômenos e estados físicos, e estados de energias, dimensões fenomênicas de Graceli.

trans-intermecânica de TUNELAMENTO no sistema categorial de Graceli.

EPG = d [hc] [T / IEEpei [pit] = [pTEMRLD] and [fao] [itd] [iicee] tetdvd [pe] cee [caG].]

p it = potentials of interactions and transformations.
Temperature divided by isotopes and physical states and potential states of energies and isotopes = emissions, random wave fluxes, ion interactions, charges and energies structures, tunnels and entanglements, transformations and decays, vibrations and dilations, electrostatic potential, conductivities, entropies and enthalpies. categories and agents of Graceli.

h e = quantum index and speed of light.

[pTEMRlD] = THERMAL, ELECTRICAL, MAGNETIC, RADIOACTIVE, Luminescence, DYNAMIC POTENTIAL] ..

EPG = GRACELI POTENTIAL STATUS.

[pTFE] = POTENCIAL DE TRANSIÇÕES DE FASES DE ESTADOS FÍSICOS E DE ENERGIAS E FANÔMENOS [TRANSIÇÕES DE GRACELI]

, [pTEMRLD] [hc] [pI] [PF] [pIT][pTFE] [CG]..

{\vec {B}}_{({\vec {r}})}={\frac {\mu }{4\pi }}{\frac {1}{r^{3}}}[3({\vec {m}}.{\vec {\hat {r}}}){\vec {\hat {r}}}-{\vec {m}}]

X

T l T l E l Fl dfG l

N l El tf l

P l Ml tfefel

Ta l Rl

Ll

Dl

{\vec {F}}=\nabla ({\vec {m}}.{\vec {B}})

X

T l T l E l Fl dfG l

N l El tf l

P l Ml tfefel

Ta l Rl

Ll

Dl

d{\vec {B}}=k{\frac {i{\vec {ds}}\times {\vec {u_{r}}}}{r^{2}}}=k{\frac {i{\vec {ds}}\times {\vec {r}}}{r^{3}}}

X

T l T l E l Fl dfG l

N l El tf l

P l Ml tfefel

Ta l Rl

Ll

Dl

{\vec {B}}={\frac {\mu }{4\pi }}\int {d{\vec {B}}}={\frac {\mu }{4\pi }}\int {\frac {i{\vec {ds}}\times {\vec {u_{r}}}}{r^{2}}}={\frac {\mu }{4\pi }}\int {\frac {i{\vec {ds}}\times {\vec {r}}}{r^{3}}}

X

T l T l E l Fl dfG l

N l El tf l

P l Ml tfefel

Ta l Rl

Ll

Dl

{\vec {dF}}={\frac {\mu }{4\pi }}.{\frac {i'{\vec {ds'}}\times i{\vec {ds}}\times {\vec {u_{r}}}}{r^{2}}}

X

T l T l E l Fl dfG l

N l El tf l

P l Ml tfefel

Ta l Rl

Ll

Dl

{\vec {F}}=\int {\vec {dF}}=\int i'{\vec {ds'}}\times {\vec {B}}_{({\vec {r}})}

X

T l T l E l Fl dfG l

N l El tf l

P l Ml tfefel

Ta l Rl

Ll

Dl

\oint _{perim.}{\vec {B}}{\vec {dl}}=\mu _{0}\int _{sup.}{\vec {j}}{\vec {da}}=\mu _{0}I_{enc.}

X

T l T l E l Fl dfG l

N l El tf l

P l Ml tfefel

Ta l Rl

Ll

Dl

\int _{sup.}(\nabla \times {\vec {v}}).{\vec {da}}=\oint _{perim.}{\vec {v}}.{\vec {dl}}

X

T l T l E l Fl dfG l

N l El tf l

P l Ml tfefel

Ta l Rl

Ll

Dl

\nabla \times {\vec {B}}=\mu _{0}{\vec {j}}

X

T l T l E l Fl dfG l

N l El tf l

P l Ml tfefel

Ta l Rl

Ll

Dl

\oint _{sup.}{\vec {B}}{\vec {da}}=0

X T l T l E l Fl dfG l N l El tf l P l Ml tfefel Ta l Rl Ll Dl

\oint _{perim.}{\vec {B}}{\vec {dl}}=\mu _{0}\int _{sup.}{\vec {j}}{\vec {da}}=\mu _{0}I_{enc.}

X T l T l E l Fl dfG l N l El tf l P l Ml tfefel Ta l Rl Ll Dl

{\vec {B}}={\frac {\mu _{0}I}{2\pi r}}{\vec {u_{\theta }}}

X T l T l E l Fl dfG l N l El tf l P l Ml tfefel Ta l Rl Ll Dl

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